US4000458A - Method for the noncontacting measurement of the electrical conductivity of a lamella - Google Patents
Method for the noncontacting measurement of the electrical conductivity of a lamella Download PDFInfo
- Publication number
- US4000458A US4000458A US05/606,365 US60636575A US4000458A US 4000458 A US4000458 A US 4000458A US 60636575 A US60636575 A US 60636575A US 4000458 A US4000458 A US 4000458A
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- United States
- Prior art keywords
- lamella
- measurement
- conductivity
- approximately
- inductor
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Links
- 238000005259 measurement Methods 0.000 title claims abstract description 39
- 241000446313 Lamella Species 0.000 title claims abstract description 18
- 238000000034 method Methods 0.000 title claims description 32
- 239000004065 semiconductor Substances 0.000 claims abstract description 15
- 235000012431 wafers Nutrition 0.000 claims abstract description 9
- 229910052751 metal Inorganic materials 0.000 claims abstract description 8
- 239000002184 metal Substances 0.000 claims abstract description 8
- 239000003990 capacitor Substances 0.000 claims description 3
- 230000010355 oscillation Effects 0.000 abstract description 16
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- 239000000523 sample Substances 0.000 description 28
- 239000000463 material Substances 0.000 description 7
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- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
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- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
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- 239000010931 gold Substances 0.000 description 1
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Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
- G01N27/02—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance
- G01N27/023—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance where the material is placed in the field of a coil
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
- G01R27/02—Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
- G01R27/26—Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants ; Measuring impedance or related variables
Definitions
- the invention is in the field of electronic solid state device processing, more particularly, semiconductor wafer or metal thin film conductivity measurement.
- the ability to rapidly and accurately measure the electric conductivity of thin flat samples is of critical importance in many aspects of solid state device processing. Such measurements are essential parts of the classification of semiconductor substrate materials prior to processing, to the monitoring of dopant diffusions and the monitoring of metal thin film depositions.
- the most widely used measurement technique is the four point probe method. However this method has several limitations, for example, it is difficult to interpret the results of such a measurement made on high resistivity semiconductor samples.
- the probe causes localized surface damage at the point of contact. Such surface damage becomes more and more detrimental as the element size of microminiature circuits becomes smaller.
- Noncontacting techniques for the measurement of electrical conductivity have been developed in an effort to avoid the limitations of the four point probe technique. These methods generally involve the interaction of the sample being measured with high frequency excitations. Exemplary techniques of this class include: microwave transmission measurements through a semiconductor slab placed in a waveguide (H. Jacobs et al. Proceedings of the IRE, 49 (1961) 928); reflection of an RF signal from a coaxial line terminated by the sample (C. A. Bryant et al. Reviews of Scientific Instruments, 26 (1965)1614); and capacitive coupling and inductive coupling to a resonant circuit (N. Nuyamoto et al. Reviews of Scientific Instruments, 38 (1967) 360; J. C. Brice et al.
- Such methods typically produce nonlinear output signals which require calibration over the range of use and comparison of the measurement signals to the calibration curve.
- measurements have typically made use of some relatively ill defined measurement volume (e.g., approximately hemispherical), which may be quite satisfactory for the measurement of uniformly conductive samples, however, increase the complexity of analysis of measurement results for nonuniform samples (e.g., diffused layers in semiconductors).
- a noncontacting technique has been developed for the measurement of the electrical conductivity of thin flat samples (lamellae) such as semiconductor wafers or metal thin films.
- This technique produces a highly linear output signal and measures the conducting carriers uniformly through the thickness of the material.
- This high degree of linearity together with the ability to control the level of the output signal can be used to produce the direct reading of conductivity on, for example, a digital voltmeter.
- This capability makes the inventive technique particularly attractive for production line monitoring of diffusions and depositions in substrates in electronic device processing.
- the sample is introduced into the magnetic field of the inductive element of a resonant circuit and the drive current of the resonator is adjusted to restore the amplitude of oscillation to the value it had prior to introduction of the sample.
- the frequency of oscillation is selected to make skin effect negligible and if the resonator is the frequency determining element of the oscillation circuit, then the incremental current is linearly related to the sheet conductivity of the sample.
- feedback is used to automatically restore the oscillation amplitude. This exemplary apparatus was linear within approximately 1% over a 100 to 1 range of conductivity with a resolution of approximately one part in 10 4 .
- the limiting sensitivity of the instrument was ⁇ 10 11 carriers per square centimeter.
- FIG. 1 is a schematic representation of the basic elements of a device for the practice of the claimed method
- FIG. 2 is a circuit diagram of an exemplary network developed for the practice of the claimed process
- FIG. 3 is an elevational view in section of an exemplary inductor with sample
- FIG. 4 is an exploded perspective view of the mechanical parts of an exemplary apparatus developed for the practice of a claimed process.
- FIG. 5 is a curve of sheet conductivity (ordinate) vs output signal (abscissa) illustrating the linearity of the inventive method.
- the measurement of the electrical conductivity (or resistivity) of broad thin solid bodies is of major importance in many facets of solid state device processing. For example it is usually necessary to classify semiconductor substrates prior to processing to make sure that the conductivity of the substrates is either less than a specified low value or within some narrow conductivity range. During processing it is usually necessary to monitor diffusion steps to determine when the conductivity of the diffused wafers has increased or decreased to some conductivity with a narrow range, which is related to the desired dopant concentration and diffusion depth. Many diffusions are caused to take place through apertured masking layers. In such cases a blank wafer can be included for monitoring purposes. Most solid state device processes includes the deposition of metal layers for the production of electrical contact between devices in an integrated circuit or between the circuit and external circuitry.
- the layer must be thicker than some minimum thickness, in order to provide sufficient conductivity, but not unnecessarily thick, so as to be wasteful of precious metals such as gold and platinum.
- the monitoring of metal layer thickness becomes an important manufacturing process step.
- the most widely used method for making the required conductivity measurements is the four point probe technique.
- these methods are exceedingly difficult because the contacts between the wafer being measured and the contacting elements of the four point probe tend to be rectifying.
- some diffusions take place through glassy layers making it difficult to contact the underlying semiconductor.
- the four point probe since it directly contacts the material, produces localized damage. The damaged area can be made unsuitable for use, particularly for devices with small element size. The above considerations make the development of a noncontacting method particularly desirable.
- the herein disclosed noncontacting method for the electrical conductivity measurement of conducting lamellae produces a highly linear output. This makes possible, for example, single point calibration and, with the availability of signal level adjustment, the direct reading of conductivity on a digital voltmeter.
- the measurement method can be understood with reference to FIG. 1 which shows a conductive lamella 11 magnetically coupled by means of a ferrite core 12 to an L-C resonant tank circuit 13. This parallel resonant circuit 13 is driven by an RF current generator 14. Operation of the measurement method depends upon the fact that eddy current absorption in the conducting lamella 11 produces an increase in the loss of the resonant circuit 13.
- the resonant circuit 13 determines the frequency of oscillation so that the frequency shifts with the loading of the circuit 13 and the frequency of oscillation is selected such that skin effect in the lamella is negligible and the current generator 14 is adjusted to restore the amplitude of oscillation after sample insertion, then the incremental current flowing from the current generator 14 into the resonant circuit 13 is linearly related to the product of the bulk conductivity of the conducting material multiplied by the thickness of the material.
- This product is sometimes referred to as the sheet conductivity of the sample and is related to the product of the number of carriers in the measured volume and the carrier mobility.
- the product of conductivity times thickness generalizes to the integral of the conductivity through the thickness so that data for nonuniform samples can be easily analyzed.
- the basic relationship which governs the measurement process is
- FIG. 2 shows the circuit diagram of an exemplary circuit developed and constructed for the practice of the inventive method. Unless otherwise specified the resistors and 1/4 watt and ⁇ 5%.
- the diodes are 1N4154, the NPN transistors are 2N3904, the PNP transistors are 2N3906, the FET's are 2N4393 and the differential amplifiers are high gain ( ⁇ 10 5 at DC, unity at 1 MHz) units suitable for use as operational amplifiers (Type 741).
- Box I outlined by dashed line 21 includes the resonant tank circuit 22 and the several transistors which form the RF current generator. These elements are arranged to form an amplitude controllable marginal oscillator whose frequency of oscillation is determined by the tank circuit 22.
- the sample to be measured is magnetically coupled to the inductor 23.
- a description of the operation of this type of oscillator can be found in Journal of Scientific Instruments, 36 (1959) 481.
- a feature of the oscillator design of FIG. 2 is that the average DC current flowing to ground on the grounded side of the tank circuit 22 is an accurate measure of the magnitude of the oscillation frequency drive current.
- the magnitude of the oscillation of the tank circuit 22 is automatically adjusted by feedback through the stabilization circuitry of Box II outlined by dashed line 24.
- the level of oscillation at the collector of transistor 37 is sensed by the temperature compensated peak rectifier formed by transistors 38 and 39, resulting in a corresponding negative voltage at the emitter of 39.
- the error amplifier 402 then senses the difference between the resulting current flowing in resistor 40 and the reference current flowing in resistor 401.
- the stabilization reference is an 8 volt zener diode 26.
- the tank circuit oscillation amplitude is thereby sensed through lead 27 and the feedback control is supplied by lead 28.
- the average DC tank circuit current is measured at lead 29 by the action of amplifier 30.
- the output circuitry includes a gain control pot 31, a range switch 32 and an overrange indicator lamp 33, which lights to indicate the presence of a sample whose conductivity is above the two decade range of the instrument.
- Amplifier 34 and a precision ten turn potentiometer 35 are arranged so as to accomplish the division of the thickness of the material prior to extraction of the conductivity signal in the output port 36. The gain is adjusted so that potentiometer 35 reads directly in convenient units of sample thickness.
- the components labeled with an asterisk have values that are selected depending upon the particular choice of input tank circuit, L 1 C 1 . The values indicated are those for an instrument reading out at one volt per mho-cm.sup.
- the design of the inductor is illustrated in FIG. 3.
- the inductor core design was chosen to be a split high Q ferrite cup core 41 with two turns in each half, resulting in a total inductance of approximately 1 ⁇ h.
- the cores employed are characterized by a permeability of ⁇ 100 and a Q of ⁇ 100 at the 10MHz oscillation frequency.
- the number of turns 42 can be changed to 20 or 200 etc. to achieve corresponding 10 2 and 10 4 range scaling as indicated by the 1/n 2 dependence of Equation 1. If C 1 remains unchanged the attendant reduction of oscillation frequency helps to satisfy the skin effect criterion for the measurement of higher conductivity samples 43.
- the inductor design also includes seamless aluminum cups 44 which reduce the fringing field and maintain the measurement area precisely and exclusively as the region between the opposing faces of the two core halves. Capacitive coupling to the sample 43 is minimized by the inclusion of an electrostatic shield 45 over the faces of the cores 41.
- the shield used was an electrically conductive paper (available from Western Union Corp. as TELEDELTOS paper).
- the mechanical design of the sample measuring head of the constructed instrument is illustrated in exploded view, in FIG. 4.
- the cup cores 41, the windings 42 and aluminum cups 44 are mounted in polymethylmethacrylate holders 46.
- the holders 46 are bolted onto the base such that shims 47 can be inserted to adjust the gap between the cores to accommodate various sample 43 thicknesses.
- the leads 48 from the inductor are shielded and lead downward into case 49 containing the electronic circuitry and connected to the tank circuit capacitor 50.
- Similar instruments for the measurement of higher conductivity semiconductor wafers i.e., in the 5 mho-cm.sup. -1 to 10 3 mho-cm.sup. -1 range
- the operating frequency of such instruments is approximately 10 6 Hz.
- cup cores with 10 3 turns on each side, together with a 0.01 ⁇ f capacitor produces an instrument oscillating at approximately 10 4 Hz.
- Resistor 25 should be selected to give an overall zero reading near the center of the zeroing potentiometer 403.
- the limiting performance of the instrument was set by slow long term drifts of the order of a few millivolts per hour corresponding to a few parts in 10 4 of the system full scale output of approximately 10 volts. The readings were stable and reproducible to this accuracy. Subsequent analysis of the circuit indicated that it may be possible to reduce these drifts by operating at higher oscillator drive levels and eliminating the amplification at the output of the tank circuit 22 (amplifier 30).
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Biochemistry (AREA)
- Immunology (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Analytical Chemistry (AREA)
- Chemical Kinetics & Catalysis (AREA)
- General Health & Medical Sciences (AREA)
- Electrochemistry (AREA)
- Pathology (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Testing Or Measuring Of Semiconductors Or The Like (AREA)
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Priority Applications (11)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US05/606,365 US4000458A (en) | 1975-08-21 | 1975-08-21 | Method for the noncontacting measurement of the electrical conductivity of a lamella |
| CA256,881A CA1057823A (en) | 1975-08-21 | 1976-07-13 | Method for the noncontacting measurement of the electrical conductivity of a lamella |
| SE7608925A SE410901B (sv) | 1975-08-21 | 1976-08-10 | Forfarande for icke-kontaktande metning av den elektriska konduktiviteten hos en bricka |
| BE169834A BE845220A (fr) | 1975-08-21 | 1976-08-16 | Procede de mesure de la conductivite d'une lamelle sans contact avec celle-ci |
| FR7624912A FR2321702A1 (fr) | 1975-08-21 | 1976-08-16 | Procede de mesure de la conductivite d'une lamelle sans contact avec celle-ci |
| DE2636999A DE2636999C3 (de) | 1975-08-21 | 1976-08-17 | Verfahren zum berührungslosen Messen der spezifischen elektrischen Leitfähigkeit eines Plättchens |
| NL7609128.A NL168051B (nl) | 1975-08-21 | 1976-08-17 | Werkwijze voor het niet-contacterend meten van de elek- trische geleidbaarheid van een lamelvormig voorwerp, onder toepassing van het wervelstroomverliesbeginsel. |
| JP9826976A JPS5319874A (en) | 1975-08-21 | 1976-08-19 | Method of measuring electric conductivity of sheet without touching |
| GB34741/76A GB1552948A (en) | 1975-08-21 | 1976-08-20 | Measuring the electrical conductivity of a lamella |
| ES450860A ES450860A1 (es) | 1975-08-21 | 1976-08-20 | Procedimiento para la medicion sin contacto de la conducti- vidad electrica de una laminilla. |
| IT69068/76A IT1071415B (it) | 1975-08-21 | 1976-08-20 | Procedimento per la fabbricazione di oggetti lamellari..particolarmente sottostrati semiconduttori o lamelle metalliche |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US05/606,365 US4000458A (en) | 1975-08-21 | 1975-08-21 | Method for the noncontacting measurement of the electrical conductivity of a lamella |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US4000458A true US4000458A (en) | 1976-12-28 |
Family
ID=24427675
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US05/606,365 Expired - Lifetime US4000458A (en) | 1975-08-21 | 1975-08-21 | Method for the noncontacting measurement of the electrical conductivity of a lamella |
Country Status (11)
| Country | Link |
|---|---|
| US (1) | US4000458A (enExample) |
| JP (1) | JPS5319874A (enExample) |
| BE (1) | BE845220A (enExample) |
| CA (1) | CA1057823A (enExample) |
| DE (1) | DE2636999C3 (enExample) |
| ES (1) | ES450860A1 (enExample) |
| FR (1) | FR2321702A1 (enExample) |
| GB (1) | GB1552948A (enExample) |
| IT (1) | IT1071415B (enExample) |
| NL (1) | NL168051B (enExample) |
| SE (1) | SE410901B (enExample) |
Cited By (68)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4075557A (en) * | 1975-10-01 | 1978-02-21 | Ckd Praha, Oborovy Podnik | Contactless facilities for determining the specific resistance of a test sample |
| US4142145A (en) * | 1977-12-22 | 1979-02-27 | The United States Of America As Represented By The Secretary Of The Navy | Method for determining conduction-band edge and electron affinity in semiconductors |
| US4144488A (en) * | 1977-12-22 | 1979-03-13 | The United States Of America As Represented By The Secretary Of The Navy | Investigation of near-surface electronic properties in semiconductors by electron beam scanning |
| US4286215A (en) * | 1979-05-18 | 1981-08-25 | Bell Telephone Laboratories, Incorporated | Method and apparatus for the contactless monitoring carrier lifetime in semiconductor materials |
| US4353029A (en) * | 1978-02-13 | 1982-10-05 | Ade Corporation | Self inverting gauging system |
| US4428782A (en) | 1982-07-23 | 1984-01-31 | The Electricity Council | Production of aluminium alloy strip |
| US4591707A (en) * | 1978-10-18 | 1986-05-27 | Gao Gessellschaft Fur Automation Und Organisation Mbh | Printed security with hallmarks |
| US4779739A (en) * | 1981-12-04 | 1988-10-25 | Gte Products Corporation | Method and apparatus for conductive film detection |
| US4797614A (en) * | 1984-11-02 | 1989-01-10 | Sierracin Corporation | Apparatus and method for measuring conductance including a temperature controlled resonant tank circuit with shielding |
| US4842147A (en) * | 1981-12-04 | 1989-06-27 | Gte Products Corporation | Method and apparatus for conductive film detection |
| DE3815010A1 (de) * | 1988-04-30 | 1989-11-09 | Leybold Ag | Schaltungsanordnung fuer den kombinierten einsatz einer induktiven und einer kapazitiven einrichtung fuer die zerstoerungsfreie messung des ohmschen wiederstands duenner schichten |
| EP0337253A3 (en) * | 1988-04-13 | 1990-12-19 | Department Of Energy Government Of The United States | Apparatus and method for characterizing conductivity of materials |
| US5394084A (en) * | 1991-12-23 | 1995-02-28 | The Boeing Company | Method and apparatus for reducing errors in eddy-current conductivity measurements due to lift-off by interpolating between a plurality of reference conductivity measurements |
| US5434505A (en) * | 1993-07-30 | 1995-07-18 | Litton Systems, Inc. | Method and apparatus for low temperature HEMT-like material testing |
| US5466614A (en) * | 1993-09-20 | 1995-11-14 | At&T Global Information Solutions Company | Structure and method for remotely measuring process data |
| US5528142A (en) * | 1995-06-19 | 1996-06-18 | Feickert; Carl A. | Resonant eddy analysis- a contactless, inductive method for deriving quantitative information about the conductivity and permeability of a test sample |
| US5552704A (en) * | 1993-06-25 | 1996-09-03 | Tencor Instruments | Eddy current test method and apparatus for measuring conductance by determining intersection of lift-off and selected curves |
| US6448795B1 (en) * | 1999-02-12 | 2002-09-10 | Alexei Ermakov | Three coil apparatus for inductive measurements of conductance |
| US6476604B1 (en) * | 1999-04-12 | 2002-11-05 | Chartered Semiconductor Manufacturing Ltd. | Method and apparatus for identifying high metal content on a semiconductor surface |
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| RU2424532C1 (ru) * | 2010-03-12 | 2011-07-20 | Государственное образовательное учреждение высшего профессионального образования Читинский государственный университет (ЧитГУ) | Способ учета электрической энергии |
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| RU2442178C2 (ru) * | 2009-06-29 | 2012-02-10 | Учреждение Российской академии наук Институт радиотехники и электроники им. В.А. Котельникова РАН | Способ определения частоты узкополосного сигнала |
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| US9631919B2 (en) | 2013-06-12 | 2017-04-25 | Applied Materials, Inc. | Non-contact sheet resistance measurement of barrier and/or seed layers prior to electroplating |
| US9754846B2 (en) | 2014-06-23 | 2017-09-05 | Applied Materials, Inc. | Inductive monitoring of conductive trench depth |
| US9911664B2 (en) | 2014-06-23 | 2018-03-06 | Applied Materials, Inc. | Substrate features for inductive monitoring of conductive trench depth |
| US10350723B2 (en) | 2016-09-16 | 2019-07-16 | Applied Materials, Inc. | Overpolishing based on electromagnetic inductive monitoring of trench depth |
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| US11231392B2 (en) | 2016-12-27 | 2022-01-25 | Industrial Technology Research Institute | Detecting device and method thereof |
| CN114113789A (zh) * | 2021-11-25 | 2022-03-01 | 天津大学 | 一种高频下测量金属薄膜电导率的装置及方法 |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0007408A1 (fr) * | 1978-07-14 | 1980-02-06 | International Business Machines Corporation | Appareil de mesure sans contact de la résistance de feuille des matériaux |
| JPS6228674A (ja) * | 1985-07-30 | 1987-02-06 | Shinetsu Eng Kk | 半導体ウエ−ハの導電率の非接触測定方法およびその装置 |
| DE3815011A1 (de) * | 1988-04-30 | 1989-11-16 | Leybold Ag | Einrichtung zum zerstoerungsfreien messen des ohmschen widerstands duenner schichten |
| DE3815009A1 (de) * | 1988-04-30 | 1989-11-09 | Leybold Ag | Einrichtung und verfahren zum zerstoerungsfreien messen des ohmschen widerstands duenner schichten nach dem wirbelstrom-prinzip |
| JPH0389331A (ja) * | 1989-09-01 | 1991-04-15 | Asahi Optical Co Ltd | カメラのシャッタ装置 |
| DE4231392A1 (de) * | 1992-09-19 | 1994-03-24 | Daimler Benz Ag | Verfahren zur Bestimmung der elektronischen Eigenschaften von Halbleiterschichtstrukturen |
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| DE2115437C3 (de) * | 1971-03-30 | 1978-04-27 | Siemens Ag, 1000 Berlin Und 8000 Muenchen | Verfahren zur berührungslosen Leitfähigkeitsmessung |
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- 1976-07-13 CA CA256,881A patent/CA1057823A/en not_active Expired
- 1976-08-10 SE SE7608925A patent/SE410901B/xx unknown
- 1976-08-16 FR FR7624912A patent/FR2321702A1/fr active Granted
- 1976-08-16 BE BE169834A patent/BE845220A/xx not_active IP Right Cessation
- 1976-08-17 NL NL7609128.A patent/NL168051B/xx not_active IP Right Cessation
- 1976-08-17 DE DE2636999A patent/DE2636999C3/de not_active Expired
- 1976-08-19 JP JP9826976A patent/JPS5319874A/ja active Granted
- 1976-08-20 IT IT69068/76A patent/IT1071415B/it active
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| US4075557A (en) * | 1975-10-01 | 1978-02-21 | Ckd Praha, Oborovy Podnik | Contactless facilities for determining the specific resistance of a test sample |
| US4142145A (en) * | 1977-12-22 | 1979-02-27 | The United States Of America As Represented By The Secretary Of The Navy | Method for determining conduction-band edge and electron affinity in semiconductors |
| US4144488A (en) * | 1977-12-22 | 1979-03-13 | The United States Of America As Represented By The Secretary Of The Navy | Investigation of near-surface electronic properties in semiconductors by electron beam scanning |
| US4353029A (en) * | 1978-02-13 | 1982-10-05 | Ade Corporation | Self inverting gauging system |
| US4591707A (en) * | 1978-10-18 | 1986-05-27 | Gao Gessellschaft Fur Automation Und Organisation Mbh | Printed security with hallmarks |
| US4691940A (en) * | 1978-10-18 | 1987-09-08 | Gao Gesellschaft Fur Automation Und Organisation Mbh | Printed security with hallmarks |
| US4286215A (en) * | 1979-05-18 | 1981-08-25 | Bell Telephone Laboratories, Incorporated | Method and apparatus for the contactless monitoring carrier lifetime in semiconductor materials |
| US4779739A (en) * | 1981-12-04 | 1988-10-25 | Gte Products Corporation | Method and apparatus for conductive film detection |
| US4842147A (en) * | 1981-12-04 | 1989-06-27 | Gte Products Corporation | Method and apparatus for conductive film detection |
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Also Published As
| Publication number | Publication date |
|---|---|
| SE7608925L (sv) | 1977-02-22 |
| DE2636999A1 (de) | 1977-03-17 |
| DE2636999B2 (de) | 1978-03-30 |
| GB1552948A (en) | 1979-09-19 |
| NL168051B (nl) | 1981-09-16 |
| CA1057823A (en) | 1979-07-03 |
| BE845220A (fr) | 1976-12-16 |
| NL7609128A (nl) | 1977-02-23 |
| FR2321702B1 (enExample) | 1981-09-18 |
| JPS5319874A (en) | 1978-02-23 |
| JPS5520550B2 (enExample) | 1980-06-03 |
| ES450860A1 (es) | 1977-08-16 |
| DE2636999C3 (de) | 1982-03-18 |
| IT1071415B (it) | 1985-04-10 |
| SE410901B (sv) | 1979-11-12 |
| FR2321702A1 (fr) | 1977-03-18 |
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